Tau 2018 Amsterdam Sept. 27, 2018
The Mu3e Experiment
@ PSI
searching for the neutrinoless muon decay m
+→ e
+e
-e
+Alessandro Bravar
for the Mu3e collaboration
LFV in the “Standard Model”
Flavor Conservation in the charged lepton sector : processes like
m A → e A
m → e + g
m → e e e
have not been observed yet (down to 10-13 !).In SM (mn = 0) Lepton Flavor is conserved absolutely (not by principle but by structure !) neutrino oscillations mn 0 Lepton Flavor is not anymore conserved (n oscillations)
charged LFV possible via loop diagrams, but heavily suppressed m e (or m ) via n oscillations
measurement not affected by SM processes m eee via a quantum loop
L 1 / M
WE
n M
W
4
54
4 10
W
m BR e e e M
n
m
+ - -
sin (2 ) sin (2 2 2 ) 4P m L
E
n
n
2
New Physics in m → eee
several cLFV models predict sizeable effects,
accessible to the next generation of experiments !
if cLFV seen, unambiguous signal for new physics (going beyond Dirac mn > 0)
explore physics up to the PeV scale
complementary to direct searches at LHC
Dipole (Loop Diagrams)
Supersymmetry Little Higgs Models Seesaw Models
GUT models (Leptoquarks) many other models …
Contact (Tree Diagrams)
Higgs Triplet Models
New Heavy Vector Bosons (Z’) Extra dimensions (K-K towers) many other models …
Model Comparison (m → eg and m → eee)
,2 2
1 1
dipole e ee
LFV
L m
mH J J
m +
+ +
0
effective charge LFV Lagrangian (“toy” model)
Kuno & Okada
= common effective scale
= “contact” vs “loop”g* / Z*
g
explore physics up to PeV scale
de Gouvea & Vogel
4
LFV m Decays : Experimental Signatures
kinematics :
2-body decay quasi 2-body decay 3-body decay monochromatic e+, g mono-energetic e- coplanar, Spi = 0back to back SEi = mm
backgrounds :
accidentals decay in orbit radiative decay antiprotons, pions accidentalsbeam :
continuous beam pulsed beam continuous beamnone of these decays, however, have been yet observed experimentally
Mu3e @ PSI : the Challenge
search for m
+ e
+e
-e
+with sensitivity BR ~ 10
-16(PeV scale)
(m eee)> 1000 years (
m= 2.2 ms) using the most intense DC (surface) muon beam in the world (p ~ 28 MeV/c)
suppress backgrounds below 10
-16find or exclude m
+ e
+e
-e
+at the 10
-16level
4 orders of magnitude over previous experiments (SINDRUM @ PSI)
aim for sensitivity / staged approach 10
-15in Phase I
10
-16in Phase II
(i.e. find one m
+ e
+e
-e
+decay in 10
16muon decays)
observe ~10
17m decays (over a reasonable time scale) rate ~2 x 10
9m decays / s
build a detector capable of measuring 2 x 10
9m decays / s minimum material, maximum precision
project (Phase I) approved in January 2013
6
Mu3e Baseline Design – Phase I
thin (< 0.1% X
0), fast, high resolution detectors
(minimum material, maximum precision)
175 M HV-MAPS channels (Si pixels w/ embedded amplifiers) 10 k ToF channels (SciFi and Tiles)
acceptance ~ 70% for m
+ e
+e
-e
+decay (3 tracks!)
solenoid B = 1 T
surface m
p ~ 28 MeV/c 10
8m / s
~15cm
~1.2 m
Phase I
scintillating tiles scintillating fibers Si pixels (HV-MAPS)
Muons @ PSI
most intense DC muon beam590 MeV/c proton cyclotron, 1.4 MW
pE5 beamline ~ 108 m / s - surface muons ~ 28 MeV/c
- high intensity monochromatic beam (ΔP/P < 8% FWHM)
- polarization ~ 90%
(MEG exp., Mu3e phase I)
SINQ (spallation neutron source) could even provide 5 x 1010 m / s
High-intensity Muon Beamline (HiMB)
e / m 12 cm separation at last collimator
> 8σ separation
8
Mu3e – Phase I
MEGII and Mu3e (phase I)
have similar beam requirements and will share he same beam-line
Mu3e
MEG
pE5 beamline
can easily switch between the two experiments intensity O(108 muon/s)
low momentum p = 28 MeV/c small straggling
good identification of the decay region Proof-of-Principle:
delivered 8 x 107 muon/s during 2016 test beam
Signal and Backgrounds
n
en
msignal backgrounds
internal conversion accidental
features
common vertex common vertex no common vertex Sp
i= 0, SE
i= m
mSp
i 0, SE
i< m
mSp
i 0, SE
i m
min time in time out of time
vtx< 300 mm rejecting the background requires
p< 0.5 MeV/c
t< 0.5 ns
BR (m+ e+ e- e+nenm) = 3.5 x 10-5
10
Irreducible Background
m radiative decay with internal conversion
BR (m+ e+ e- e+nenm) = 3.5 x 10-5
high momentum and energy resolution required to suppress this background
p< 0.5 MeV/c and m
m< 0.5 MeV/c
2m
+ e
+e
-e
+n
en
mfraction in signal region
as a function of m
mn
en
mSp
i 0, SE
i m
mBackground Suppression
background rejected with tracking and timing
(tracking alone not sufficient to reject accidental background)
12
The Pixel Tracker
central tracker: four layers re-curl tracker: two layers
minimum material budget: tracking in multiple scattering dominated regime
momentum resolution < 0.5 MeV/c over a large phase space geometrical acceptance ~70%
X/X
0per layer ~0.011%
re-curl stations central stations
Silicon Pixel Detector HV-MAPS
High Voltage Monolithic Active Pixel Sensors : HV-MAPS
readout logic and amplifiers embedded in the pixel n-well
thin active region (10 mm) → fast charge collection via drift
< 50 mm thickness
final pixel size 80 x 80 mm2 final chip size 2 x 2 cm2 time resolution < 15 ns efficiency > 99%
175 M pixels
radiation hard operated at –85 V
1 Gb/s LVDS readout (30 M hits /s)
Peric NIMA731 (2008) 131
14
HV-MAPS R & D
50 mm thick silicon wafer Latest prototype: MUPIX 8 ( MUPIX X)
characteristics thickness 50 mm
pixel size 80 x 80 mm2 chip size 19 x 10 mm2 performance
efficiency > 99 %
time resolution < 14 ns
full size
Timing 50 ns snapshot (readout frame): 100 m decays
additional ToF information < 500 ps
to suppress accidental backgrounds requires excellent timing
< 500 ps SciFis < 100 ps scint. tiles
16
The Timing Detectors: Fibers and Tiles
precise timing measurement: critical to reduce accidental BKGs
determine sign of re-curling tracks (SciFi) scintillating fibers (SciFi) ~250 ps, detection efficiency > 95 %
scintillating tiles ~70 ps, detection efficiency > 99 %
scintillating tiles scintillating fibers
The SciFi Detector
Requirements
high detection efficiency > 95%
time resolution < 0.5 ns
thickness X/X0 ~ 0.2 % (< 700 μm)
handle high occupancy: up to 250 KHz/fiber limited space for electronics and cabling Design
cylindrical
~12 cm diameter length ~30 cm
3 staggered layers round fibers multi-clad 250 μm round fibers
readout with Si-PM arrays on both ends MuSTiC ASIC
18
SciFi Perforomance
different fibers have been evaluated
SCSF 78 MJ, SCSF 81 MJ, NOL 11, BCF 12 w/ and w/o TiO2 coating, 3 & 4 layers, … detection efficiency > 96 % @ 0.5 phe thr
timing resolution ~200 ps (mean time)
time resolution light yield
full size SciFi ribbon prototype
Si-PM array 2 x 64 ch., 250 mm pitch common cathode
32.5 mm
Summary
Mu3e will search for the neutrinoless muon decay m → e
+e
–e
+with a sensitivity at the level of 10
-16i.e. at the PeV scale
suppress backgrounds below 10
-16(16 orders of magnitude !) Novel technologies:
HV-MAPS (Si pixels, 50 mm thickness) Si-PMs (scintillating fibers and tails)
they meet the requirements
Staged approach
Stage I (2020 – 2024)
~10
8m decays / s BR(m → eee) < 10
-15approved in January 2013
Stage II (> 2025)
~2 x 10
9m decays / s BR(m → eee) < 10
-16HiMB feasibility study already started
Construction in 2018/2019 (incl. magnet) Commissioning 2020
20
LFV Searches : Current Situation
The best limits on LFV come from PSI
muon experiments m
+→ e
+e
-e
+BR < 1 x 10
-12SINDRUM 1988 m
-+ Au → e
-+ Au BR < 7 x 10
-13SINDRUM II 2006 m
+→ e
++ g
BR < 4.2 x 10
-13MEG 2016
Mu3e m
+→ e
+e
-e
+Phase I : BR < 10
-15Phase II: BR < 10
-16SINDRUM
SINDRUM II MEG
SINDRUM @ PSI (~ 80s)
e+ spectrum m+ → e+2n 105.7 MeV
3e2 0
i i i i
K E
m
p c
m
m n
+
prompt events
beam (pE3 beamline @ PSI):
5 ´ 106 m / sec
28 MeV/c surface muons resolution:
(pT) = 0.7 MeV/c2 vertex ~ 1 mm
statistics limited!
m m
ee e en n
m e
10 12 (90% CL)+ + - +
-
+ +
accidental events (normalized)
22